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Superintegrability on N-dimensional spaces of constant curvature from so(N+1) and its contractions

机译:从so(N + 1)开始的N常维曲率空间及其压缩性

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摘要

The Lie-Poisson algebra so(N + 1) and some of its contractions are used to construct a family of superintegrable Hamiltonians on the N-dimensional spherical, Euclidean, hyperbolic, Minkowskian, and (anti-)de Sitter spaces. We firstly present a Hamiltonian which is a superposition of an arbitrary central potential with N arbitrary centrifugal terms. Such a system is quasi-maximally superintegrable since this is endowed with 2N - 3 functionally independent constants of motion (plus the Hamiltonian). Secondly, we identify two maximally superintegrable Hamiltonians by choosing a specific central potential and finding at the same time the remaining integral. The former is the generalization of the Smorodinsky-Winternitz system to the above six spaces, while the latter is a generalization of the Kepler-Coulomb potential, for which the Laplace-Runge-Lenz N vector is also given. All the systems and constants of motion are explicitly expressed in a unified form in terms of ambient and polar coordinates as they are parametrized by two contraction parameters (curvature and signature of the metric).
机译:Lie-Poisson代数so(N +1)及其某些压缩用于在N维球面,欧几里得,双曲,Minkowskian和(反)de Sitter空间上构造一族超可积哈密顿量。我们首先提出一个哈密顿量,它是任意中心势与N个任意离心项的叠加。这样的系统具有2N-3个功能独立的运动常数(加上哈密顿量),因此是拟最大可积的。其次,我们通过选择特定的中心势并同时找到剩余的积分来确定两个最大超可积的哈密顿量。前者是Smorodinsky-Winternitz系统对上述六个空间的推广,而后者是Kepler-Coulomb势的推广,为此还给出了Laplace-Runge-Lenz N向量。所有的运动系统和运动常数都通过环境和极坐标以统一的形式明确表示,因为它们由两个收缩参数(曲率和度量标准)参数化。

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